Abstract:We present a new scheme to estimate the elastic properties of biological membranes in computer simulations. The method analyzes the thermal fluctuations in terms of a coupled undulatory mode, which disentangle the mixing of the mesoscopic undulations and the high-q protrusions. This approach makes possible the accurate estimation of the bending modulus both for membranes under stress and in tensionless conditions; it also extends the applicability of the fluctuation analysis to the small membrane areas normall… Show more
“…For example, for a cell membrane tension in the order of 0.05 mNÁm ¡1 and bending modulus values of 15 k B T, the length scale is approximately 50 nm [48]. Simulation [59] and experiment [60] suggest a bending modulus of k » 23 k B T (»10 ¡19 J at 300 K for DPPC gives »60 nm. In what follows, we assume k ¼ 23 k B T (unless otherwise stated) for the calculation of adhesion energy from the critical radius determined experimentally.…”
Engineered nanomaterials have a wide range of applications and as a result, are increasingly present in the environment. While they offer new technological opportunities, there is also the potential for adverse impact, in particular through possible toxicity. In this review, we discuss the current state of the art in the experimental characterisation of nanoparticle-membrane interactions relevant to the prediction of toxicity arising from disruption of biological systems. One key point of discussion is the urgent need for more quantitative studies of nano-bio interactions in experimental models of lipid system that mimic in vivo membranes.
“…For example, for a cell membrane tension in the order of 0.05 mNÁm ¡1 and bending modulus values of 15 k B T, the length scale is approximately 50 nm [48]. Simulation [59] and experiment [60] suggest a bending modulus of k » 23 k B T (»10 ¡19 J at 300 K for DPPC gives »60 nm. In what follows, we assume k ¼ 23 k B T (unless otherwise stated) for the calculation of adhesion energy from the critical radius determined experimentally.…”
Engineered nanomaterials have a wide range of applications and as a result, are increasingly present in the environment. While they offer new technological opportunities, there is also the potential for adverse impact, in particular through possible toxicity. In this review, we discuss the current state of the art in the experimental characterisation of nanoparticle-membrane interactions relevant to the prediction of toxicity arising from disruption of biological systems. One key point of discussion is the urgent need for more quantitative studies of nano-bio interactions in experimental models of lipid system that mimic in vivo membranes.
“…[14][15][16] It has been traditionally considered mainly in the context of biological membranes and soft condensed matter. The great complexity of these systems has hindered a microscopic approach based on realistic descriptions of the interatomic interactions.…”
Path-integral molecular dynamics (PIMD) simulations have been carried out to study the influence of quantum dynamics of carbon atoms on the properties of a single graphene layer. Finitetemperature properties were analyzed in the range from 12 to 2000 K, by using the LCBOPII effective potential. To assess the magnitude of quantum effects in structural and thermodynamic properties of graphene, classical molecular dynamics simulations have been also performed. Particular emphasis has been laid on the atomic vibrations along the out-of-plane direction. Even though quantum effects are present in these vibrational modes, we show that at any finite temperature classical-like motion dominates over quantum delocalization, provided that the system size is large enough. Vibrational modes display an appreciable anharmonicity, as derived from a comparison between kinetic and potential energy of the carbon atoms. Nuclear quantum effects are found to be appreciable in the interatomic distance and layer area at finite temperatures. The thermal expansion coefficient resulting from PIMD simulations vanishes in the zero-temperature limit, in agreement with the third law of thermodynamics.
“…14 The mean area of the undulatory surface area A U = ⟨A U ⟩ is often used to represent the fluctuating bilayer membrane. 12,13 Following the capillary wave theory, [26][27][28] …”
Section: Fluctuation Modes Of Bilayer Membranesmentioning
confidence: 99%
“…In our previous work, 14 we employed a Berendsen semiisotropic barostat to simulate bilayers at different surface tensions. This barostat does not produce the correct statistical ensemble and therefore it is not possible to compute the area compressibility modulus from a fluctuation analysis of the membrane area.…”
Section: Model and Simulation Detailsmentioning
confidence: 99%
“…This approach is based on our recent analysis of the spectrum of elastic deformations in a bilayer membrane. 14 …”
We present a new computational approach to quantify the area per lipid and the area compressibility modulus of biological membranes. Our method relies on the analysis of the membrane fluctuations using our recently introduced coupled undulatory (CU) mode [Tarazona et al., J. Chem. Phys. 139, 094902 (2013)], which provides excellent estimates of the bending modulus of model membranes. Unlike the projected area, widely used in computer simulations of membranes, the CU area is thermodynamically consistent. This new area definition makes it possible to accurately estimate the area of the undulating bilayer, and the area per lipid, by excluding any contributions related to the phospholipid protrusions. We find that the area per phospholipid and the area compressibility modulus features a negligible dependence with system size, making possible their computation using truly small bilayers, involving a few hundred lipids. The area compressibility modulus obtained from the analysis of the CU area fluctuations is fully consistent with the Hooke's law route. Unlike existing methods, our approach relies on a single simulation, and no a priori knowledge of the bending modulus is required. We illustrate our method by analyzing 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine bilayers using the coarse grained MARTINI force-field. The area per lipid and area compressibility modulus obtained with our method and the MARTINI forcefield are consistent with previous studies of these bilayers. C 2015 AIP Publishing LLC. [http://dx
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